JPS62245329A - Position detecting device - Google Patents

Position detecting device

Info

Publication number
JPS62245329A
JPS62245329A JP61087195A JP8719586A JPS62245329A JP S62245329 A JPS62245329 A JP S62245329A JP 61087195 A JP61087195 A JP 61087195A JP 8719586 A JP8719586 A JP 8719586A JP S62245329 A JPS62245329 A JP S62245329A
Authority
JP
Japan
Prior art keywords
magnetic
position detection
circuit
value
signal
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP61087195A
Other languages
Japanese (ja)
Inventor
Tsugunari Yamanami
山並 嗣也
Yoshinori Taguchi
田口 義徳
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Wacom Co Ltd
Original Assignee
Wacom Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Wacom Co Ltd filed Critical Wacom Co Ltd
Priority to JP61087195A priority Critical patent/JPS62245329A/en
Publication of JPS62245329A publication Critical patent/JPS62245329A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To simplify the constitution of a position detecting part by detecting a position through the use of a resistance value varying corresponding to a magnetic bias quantity applied on a magnetic substance. CONSTITUTION:A position detecting device is constituted of a position detecting part 10 consisting of lengthy shape magnetic substance 11a-11h arranged in parallel keeping a prescribed space with each other, an input pen 20 which generates a magnetic bias, a conversion circuit 30, a signal selection circuit 40 which switches and connects the conversion circuit 30, and the above stated magnetic substance 11a-11h, and a position detection circuit 50. And by positioning one end of the input pen 20 on the upper parts of the magnetic substance 11a-11h, and applying the magnetic bias from the tip of the pen, the resistance value R of each of the magnetic substance 11a-11h shows the minimum value for the magnetic substance 11 positioned nearest to the position, and the values go higher gradually as they are separated from the position. In this way, respective voltage of each of the magnetic substance 11a-11h in an X direction is taken out at the position detection circuit 50, from the state of the resistance value R, and a voltage value having the minimum value is found by performing an arithmetic operation, thereby the coordinate value of the input pen 20 being decided.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、磁気発生蒸により1&弄を加えられた磁性体
のインピーダンス、特に抵抗値の変化に基づいて、指定
された位置を検出する位置検出装置に関するものである
Detailed Description of the Invention (Field of Industrial Application) The present invention provides a method for detecting a specified position based on a change in the impedance, particularly the resistance value, of a magnetic material that has been subjected to magnetic generation and evaporation. This invention relates to a detection device.

(従来の技術) 従来の位置検出装置としては、磁歪伝達媒体の一端また
は位置指示ベンの先端に設けた駆動コイルにパルス電流
を印加して前記磁歪伝達媒体に磁歪振動波を生起させた
時点より、位置指示ペンの先端または磁歪伝達媒体の一
端に設けた検出コイルに前記磁歪振動波に基づく誘導゛
磁圧を検出するまでの時間を処理器等で測定し、これよ
り位置指示ペンの指示位置を算出する如くなしたものが
あった。また、従来の他の位置検出装置としては、複数
の駆動線と検出線とを互いに直交して配置し、駆動線に
順次、電流を流すとともに検出線を順次選択して誘導電
圧を検出し、フェライトのような磁性体を有する位置指
示ペンで指定した位置を大きな誘導電圧が誘起された検
出線の位置より検出するようになしたものがあった。
(Prior art) As a conventional position detection device, a pulse current is applied to a drive coil provided at one end of a magnetostrictive transmission medium or at the tip of a position indicating ben, and magnetostrictive vibration waves are generated in the magnetostrictive transmission medium. The time required to detect the induced magnetic pressure based on the magnetostrictive vibration waves in the detection coil provided at the tip of the positioning pen or one end of the magnetostrictive transmission medium is measured by a processor, etc., and from this time the indicated position of the positioning pen is determined. There was something that was done to calculate the . In addition, as another conventional position detection device, a plurality of drive lines and detection lines are arranged perpendicularly to each other, and current is sequentially applied to the drive lines and detection lines are sequentially selected to detect induced voltage. There is a device in which a position specified by a position indicating pen made of a magnetic material such as ferrite is detected from the position of a detection line where a large induced voltage is induced.

(発明が解決しようとする問題点) 前者の装置aでは位置検出精度は比較的良好であるが、
ペンと処理器等との間でタイミング信号等を授受するた
め、ペンと装置との間にコードを必要としその取扱いが
著しく制限されると共に、他の機器からの誘導を受けや
すく誤動作したり、また逆にノイズの発生源となる可能
性もあり、更にペンを磁歪伝達媒体に対して垂直に保持
し、かつかなり近接させて指示しなければならない等の
問題点があった。また、後者の装置では位置指示ペンを
コードレスとすることができるが、座標位置の分解能が
線の間隔で決まり、分解能を上げるために線の間隔を小
さくするとSN比及び安定度が悪くなり、従って分解能
を上げることが困難であり、また駆動線と検出線の交点
の真丘の位置検出が困難であり、更に位置指示ペンを線
に極く接近させなければならず入力面上に厚みのある物
を置いて使用できない等の問題点があった。
(Problems to be Solved by the Invention) Although the former device a has relatively good position detection accuracy,
In order to send and receive timing signals, etc. between the pen and the processor, etc., a cord is required between the pen and the device, and its handling is severely restricted, and it is also susceptible to guidance from other devices, causing malfunctions and In addition, there is a possibility that the pen may become a source of noise, and furthermore, there are other problems such as the need to hold the pen perpendicular to the magnetostrictive transmission medium and to point it fairly close to it. In addition, in the latter device, the positioning pen can be cordless, but the resolution of the coordinate position is determined by the spacing between the lines, and if the spacing between the lines is made small to increase the resolution, the S/N ratio and stability will deteriorate. It is difficult to increase the resolution, it is difficult to detect the position of the true ridge at the intersection of the drive line and the detection line, and the positioning pen must be placed very close to the line, making it difficult to use thick objects on the input surface. There were problems such as not being able to use it with the

本発明はこのような従来の欠点を改善したものであり、
位置指定用磁気発生器がどこにも接続されず操作性が良
く、また外部からの誘導に強く且つノイズを放出Jるこ
とのない高精度な位置検出装置を提供することを目的と
する。
The present invention improves these conventional drawbacks, and
To provide a highly accurate position detecting device which has good operability since a magnetic generator for specifying a position is not connected anywhere, is strong against external guidance, and does not emit noise.

(問題点を解決Jるための手段) 本発明の位置検出装置は、第1図に示Jように所定間隔
隔てて互いにほぼ平行に配列された複数の長尺の磁性体
118〜11[1を備えた位置検出部10と、定常的な
磁界を発生する位置指定用磁気発生器、例えば入力ペン
20と、導体のインピーダンス値を電気信号に変換する
変換回路30と、該変換回路30と前記位置検出部10
の複数の磁性体11a〜11hとを切苔え接続する信号
選択回路40と、前記位置検出部10の複数の磁性体1
18〜11hのそれぞれに対応した電気信号から前記入
力ベン20の指示位置を算出する位置検出回路50とか
らなっている。
(Means for Solving the Problems) The position detection device of the present invention has a plurality of long magnetic bodies 118 to 11[1] arranged substantially parallel to each other at predetermined intervals as shown in FIG. a position detection unit 10 equipped with a position detection unit 10, a position designating magnetic generator that generates a steady magnetic field, such as an input pen 20, a conversion circuit 30 that converts the impedance value of a conductor into an electrical signal, and the conversion circuit 30 and the Position detection section 10
a signal selection circuit 40 that connects the plurality of magnetic bodies 11a to 11h by cutting and connecting the plurality of magnetic bodies 11a to 11h;
It is comprised of a position detection circuit 50 that calculates the indicated position of the input ben 20 from electrical signals corresponding to each of 18 to 11h.

(作用) 前記磁性体11a〜11hのインピーダンス値、特に抵
抗値Rを式で表わすと、 R−(J/S)ρ となる(但し、lは磁性体の長さ、S &、を磁性体の
断面積、ρは比抵抗である。)。ここで、!、Sは使用
する磁性体11a〜Ilhの具体的な寸法によって定ま
り、変化しないと仮定できるから、前記抵抗値Rは磁性
体118〜11hの比抵抗ρに比例する。
(Function) The impedance value, especially the resistance value R, of the magnetic bodies 11a to 11h can be expressed as R-(J/S)ρ (where l is the length of the magnetic body, and S &, is the magnetic body , and ρ is the resistivity.) here,! , S are determined by the specific dimensions of the magnetic bodies 11a to 11h used and can be assumed not to change, so the resistance value R is proportional to the specific resistance ρ of the magnetic bodies 118 to 11h.

ところで、磁性体11a〜11hの比抵抗ρは外部から
加わる磁気バイアスによって大きく変化する。その変化
のようすは磁性体の組成、前記交流電流の周波数、ある
いは磁性体に熱処理、又は磁場処理を加えることなどに
よって異なるが、一般に負の特性、即ち磁気バイアスを
加えれば加える程、小さくなる性質を示す。従って、第
2図に示すように棒磁石21を内蔵する人力ペン20の
一端を磁性体11a〜11hの上部に位置させ、その先
端よ0定常的な磁界(以下、磁気バイアスと称す。)を
加えると、各磁性体118〜11hの抵抗値Rは、該入
力ベン20を置いた位置に最も近い磁性体の抵抗値を最
小値として、ここから離れるに従って徐々に大きくなる
By the way, the specific resistance ρ of the magnetic bodies 11a to 11h changes greatly depending on the magnetic bias applied from the outside. The nature of this change varies depending on the composition of the magnetic material, the frequency of the alternating current, or whether the magnetic material is subjected to heat treatment or magnetic field treatment, but generally it has a negative characteristic, that is, the more magnetic bias is applied, the smaller it becomes. shows. Therefore, as shown in FIG. 2, one end of the human-powered pen 20 containing the bar magnet 21 is positioned above the magnetic bodies 11a to 11h, and a constant magnetic field (hereinafter referred to as magnetic bias) is applied to the tip. In addition, the resistance value R of each of the magnetic bodies 118 to 11h takes the resistance value of the magnetic body closest to the position where the input ben 20 is placed as the minimum value, and gradually increases as it moves away from this value.

ここで、抵抗値Rを直接求めることも可能であるが、以
後の処理が困難であるので、変換回路30と信号選択回
路40とにより各磁性体118〜11hの抵抗値Rを電
気信号、例えば電圧に変換する。第3図は、各磁性体1
18〜llhの抵抗値Rに対応した電圧値■1〜v8を
示すもので、横軸は磁性体11a〜11hに直交する方
向(以下、これをX方向と称す。)の座標位置を示し、
縦軸は電圧を示している。なお、座標値×1〜×8は各
磁性体11a〜11hのX方向における位置を示す。位
置検出回路50で各電圧v1〜v8を取出し、これより
電圧値が最小値となるX座標値を演専処理して求めれば
、入力ペン20のX座標値XSを求めることができる。
Here, it is possible to directly obtain the resistance value R, but since the subsequent processing is difficult, the resistance value R of each of the magnetic bodies 118 to 11h is determined by an electric signal, e.g., by the conversion circuit 30 and the signal selection circuit 40. Convert to voltage. Figure 3 shows each magnetic body 1
The voltage values ■1 to v8 corresponding to the resistance values R of 18 to 11h are shown, and the horizontal axis indicates the coordinate position in the direction perpendicular to the magnetic bodies 11a to 11h (hereinafter referred to as the X direction).
The vertical axis shows voltage. Note that the coordinate values x1 to x8 indicate the positions of the respective magnetic bodies 11a to 11h in the X direction. The X coordinate value XS of the input pen 20 can be determined by extracting each of the voltages v1 to v8 with the position detection circuit 50 and calculating the X coordinate value at which the voltage value becomes the minimum value by performing mathematical processing.

また、入力ペン20を磁性体11a〜11hに沿って動
かしても、各磁性体に与える磁気バイアス団は変わらな
いので、同一のX座標値が得られる。また、2つの位置
検出部10を互いに直交させて組合せれば、X及びY方
向のいわゆる2次元座標値を求めることもできる。
Further, even if the input pen 20 is moved along the magnetic bodies 11a to 11h, the magnetic bias group applied to each magnetic body does not change, so the same X coordinate value can be obtained. Furthermore, by combining two position detection units 10 orthogonal to each other, so-called two-dimensional coordinate values in the X and Y directions can also be obtained.

座標1+TJ x 、を求める算出方法の一つとして、
第3図における極小値(ここでは最小値と同一。)付近
の波形を適当な函数で近似し、その函数の極小値の座標
を求める方法がある。例えば、各磁性体11a〜11h
の間隔をlXとし、第3図において座標×3から座標×
5までを2次函数(図中、実線で示す。)で近似すると
、次のようにして算出することができる。まず、各電圧
値と座標値より、 V3=a(x3−x、)2+b  ・・−(1)V4=
a (x4−x、)  +b   −−−−(2)V5
=a (x5−x、)  +b   −・−・・−(3
)となる。ここで、a、bは定数(a>O)である。
One of the calculation methods for determining the coordinates 1+TJ x is as follows:
There is a method of approximating the waveform near the minimum value (here, the same as the minimum value) in FIG. 3 by an appropriate function and finding the coordinates of the minimum value of the function. For example, each magnetic body 11a to 11h
Let the interval of
By approximating up to 5 using a quadratic function (indicated by a solid line in the figure), it can be calculated as follows. First, from each voltage value and coordinate value, V3=a(x3-x,)2+b...-(1)V4=
a (x4-x,) +b -----(2)V5
=a (x5−x,) +b −・−・・−(3
). Here, a and b are constants (a>O).

また、 x4−×3=ΔX         ・・・・・・(4
)x s  x 3= 2Δχ      制・・(5
)となる。(4)、 (5)式を(2)、(3)式に代
入して整理すると、 x、+=x3+ 、jx/2 ((3V3−4V4+v
5)/(v3−2V4+v5)) ・・・・・・(6) となる。従って、磁性体11c、11d、lieの抵抗
値Rに対応する電圧v 、V4.v5、および座標値×
3 (既知)から位置検出回路5oで(6)式の演算を
行なうことにより、入力ペン20のX座標値X、を算出
できる。
Also, x4−×3=ΔX (4
)x s x 3=2Δχ system...(5
). Substituting equations (4) and (5) into equations (2) and (3) and rearranging, x, +=x3+ , jx/2 ((3V3-4V4+v
5)/(v3-2V4+v5)) ......(6) It becomes. Therefore, the voltages v, V4 .corresponding to the resistance values R of the magnetic bodies 11c, 11d, lie. v5, and coordinate value ×
3 (known), the X coordinate value X of the input pen 20 can be calculated by calculating the equation (6) in the position detection circuit 5o.

なJ3、磁気バイアスが増加すればする程、抵抗値が大
きくなる磁性体の場合も同様にして検出することができ
る。
Detection can be made in the same manner in the case of a magnetic material whose resistance value increases as the magnetic bias increases.

(実施例) 第4図は位置検出部10の具体的な構成を示す斜視図で
ある。磁性体11a〜11hとしては、磁石を接近させ
ても磁化されがたく、即ち保持力が小さく、かつ透11
率の高い材料、例えば直径が約0.1uの断面円形状の
アモルファスワイヤである。アモルファスワイヤとして
は、例えば(Fe1−xCOx)7.5i1oB15(
原子%)(Xは、1”el!:coとの割合を示ずもの
で、O〜1の値をとる。)等が用いられる。また、12
は前記磁性体11a〜11hを固定する基板であって、
ガラスエポキシ等の絶縁性基板の片面に銅板を貼着した
プリント基板にエツチング加工を施し、その一端に前記
磁性体118〜11hの本数と同一、即ち8個のランド
部13a〜13hを右する導体13を形成し、他端に同
じく8個のランド状の導体14a〜1411を形成して
なるものである。
(Example) FIG. 4 is a perspective view showing a specific configuration of the position detection section 10. The magnetic bodies 11a to 11h are difficult to magnetize even when a magnet is brought close to them, that is, have a small holding force, and are transparent 11
The wire is made of a material with a high coefficient of oxidation, such as an amorphous wire with a circular cross-section and a diameter of about 0.1 u. As an amorphous wire, for example, (Fe1-xCOx)7.5i1oB15(
(atomic %) (X does not indicate the ratio with 1"el!:co, and takes a value of O to 1). Also, 12
is a substrate on which the magnetic bodies 11a to 11h are fixed,
A printed circuit board with a copper plate attached to one side of an insulating substrate made of glass epoxy or the like is etched, and at one end there are conductors having the same number as the magnetic bodies 118 to 11h, that is, eight land portions 13a to 13h. 13, and eight land-shaped conductors 14a to 1411 are similarly formed at the other end.

前記磁性体118〜11hは、その両端が前記導体13
のランド部13a〜13hおよび導体14a〜14hに
それぞれ半田付けされ、且つ、その間が前記基板12上
に接着剤等により固着され、互いに所定間隔(約511
1)Illれて平行に配設されている。なお、導体13
はその一端よりリード線15を介して変換回路30に接
続され、また、各導体14a〜14hはそれぞれリード
線16a〜16hを介して信号選択回路40に接続され
る。
Both ends of the magnetic bodies 118 to 11h are connected to the conductor 13.
are soldered to the land portions 13a to 13h and conductors 14a to 14h, respectively, and the portions between them are fixed to the substrate 12 with an adhesive or the like, and are spaced apart from each other at a predetermined interval (approximately 511 mm).
1) They are arranged parallel to each other. Note that the conductor 13
are connected from one end thereof to a conversion circuit 30 via a lead wire 15, and each of the conductors 14a to 14h is connected to a signal selection circuit 40 via lead wires 16a to 16h, respectively.

なお、磁性体として、その表面に塩化ビニル等を被覆し
たものを用いても良く、この場合には熱圧着等により基
板に固定することもできる。
Note that as the magnetic material, a material whose surface is coated with vinyl chloride or the like may be used, and in this case, it can also be fixed to the substrate by thermocompression bonding or the like.

第5図は入力ベン20の具体例を示す断面図、第6図は
その電気回路図である。同図において、22は合成樹脂
等からなるペン状の8鼎であり、その一端には先端先細
状の棒磁石21が軸方向に囲動自在に収容されている。
FIG. 5 is a sectional view showing a specific example of the input vent 20, and FIG. 6 is an electric circuit diagram thereof. In the figure, reference numeral 22 denotes a pen-shaped 8-pin made of synthetic resin or the like, and a bar magnet 21 with a tapered tip is housed in one end of the pen-shaped rod so as to be movable in the axial direction.

また、容器22の他端側には周方向に亘って透明なプラ
スチック等からなる赤外線透過窓23が設けられ、その
内側には円錐体の周面にクロムメッキ等を施した反射体
24と、赤外線発光ダイオード25とが収納されている
。26a、26bは操作スイッチで、操作スイッチ26
aは容器22の先端側の一側に取付けられ、操作スイッ
チ26bは棒磁石21の他端に対向して取付けられてい
る。また、27は信号発生回路、28は電池で、容器2
2内の適所に収納されている。
In addition, an infrared transmitting window 23 made of transparent plastic or the like is provided along the circumferential direction on the other end side of the container 22, and inside the window 23 is a reflector 24 having a conical circumferential surface coated with chrome plating or the like. An infrared light emitting diode 25 is housed therein. 26a and 26b are operation switches, and the operation switch 26
a is attached to one side of the tip side of the container 22, and an operation switch 26b is attached opposite to the other end of the bar magnet 21. Further, 27 is a signal generation circuit, 28 is a battery, and the container 2
It is stored in the appropriate place within 2.

信号発生回路27は、測定開始、位置入力等の位置検出
回路50に対する複数(ここでは3通り)の命令を幾つ
かのパルス信号の組合せによる複数のコード信号にそれ
ぞれ変換Jるもので、デコーダ27aとコード信号発生
器27bとダイオード駆動用トランジスタ27cとを備
え、操作スイッチ26a、26bのオン・オフの組合せ
に従って、コード信号を発生し、発光ダイオード25を
駆a する。而して、操作スイッチ26aをオンすると
、測定開始のコードを示す赤外線信号がダイオード25
より反射体24、透過窓23を介して発信され、そのま
まカバー29を取り付けた棒磁石21の先端を入力面に
押し当てると、該棒磁石21がスライドしてスイッチ2
6bがオンし、位置入力のコード信号を示す赤外線信号
が発信される如くなっている。
The signal generation circuit 27 converts a plurality of (in this case three) commands to the position detection circuit 50, such as measurement start and position input, into a plurality of code signals based on a combination of several pulse signals, and a decoder 27a. , a code signal generator 27b, and a diode driving transistor 27c, and generates a code signal to drive the light emitting diode 25 according to the on/off combination of the operation switches 26a and 26b. When the operation switch 26a is turned on, an infrared signal indicating a measurement start code is sent to the diode 25.
When the tip of the bar magnet 21 with the cover 29 attached is pressed against the input surface, the bar magnet 21 slides and the switch 2
6b is turned on, and an infrared signal indicating a position input code signal is transmitted.

第7図は変換回路30の具体例を示すもので、図中、3
1は積分器、32はバンドパスフィルタ、33は演算回
路である。積分器31はその入力端子34に後述する位
置検出回路50の演算処理回路からのクロックパルス(
またはこれを分周したパルス)を受け、これを積分し、
三角波信号に変換する。バンドパスフィルタ32では前
記三角波信号を正弦波信号に変換し、これを演算回路3
3に送出する。演算回路33は、演算増幅器33aと抵
抗33bとからなっており、該演算増幅器33aの反転
入力端子には抵抗33bを介して前記正弦波信号が入力
され、また、反転入力端子と出力端子との間には前記磁
性体11a〜11hのうちの1つが信号選択回路、例え
ば周知のマルチプレクサ40を介して接続され、更に非
反転入力端子は接地されている。
FIG. 7 shows a specific example of the conversion circuit 30, in which 3
1 is an integrator, 32 is a band pass filter, and 33 is an arithmetic circuit. The integrator 31 receives, at its input terminal 34, a clock pulse (
or a pulse obtained by dividing this), integrate this,
Convert to triangular wave signal. The bandpass filter 32 converts the triangular wave signal into a sine wave signal, and the arithmetic circuit 3 converts the triangular wave signal into a sine wave signal.
Send to 3. The arithmetic circuit 33 consists of an operational amplifier 33a and a resistor 33b.The sine wave signal is input to the inverting input terminal of the operational amplifier 33a via the resistor 33b, and the inverting input terminal and the output terminal are connected to each other. One of the magnetic bodies 11a to 11h is connected therebetween via a signal selection circuit, for example, a well-known multiplexer 40, and the non-inverting input terminal is grounded.

ここで、磁性体118〜llhの抵抗値をR1抵抗33
bの抵抗値をR1とし、演算回路33の入力電圧をvl
、出力電圧をv2とりると、v2 =−(R/R1) 
・vl となる。従って、R1および■1を一定とすると、出力
電圧■2は抵抗IInRに依存することになり、該抵抗
値Rが減少すると、出力電圧■2も減少する。即ち、抵
抗値Rの減少を出力電圧v2の減少として検出すること
ができる。なお、基準(入力)信号にクロックパルスを
用いたのは位置検出回路50と同期をとるためである。
Here, the resistance value of the magnetic bodies 118 to llh is set to R1 resistor 33.
The resistance value of b is R1, and the input voltage of the arithmetic circuit 33 is vl.
, taking the output voltage as v2, v2 =-(R/R1)
・vl becomes. Therefore, if R1 and (1) are constant, the output voltage (2) depends on the resistor IInR, and when the resistance value R decreases, the output voltage (2) also decreases. That is, a decrease in the resistance value R can be detected as a decrease in the output voltage v2. Note that the reason why a clock pulse is used as the reference (input) signal is to synchronize with the position detection circuit 50.

第8図は位置検出回路50の具体的構成を示す回路ブロ
ック図である。同図にJ3いて、前述した入力ベン20
の発光ダイオード25より、測定開始の]−ドを示ず赤
外線信号が発信されると、該赤外線信号(よ赤外線受光
ダイオード51で受信され、更に受信機52で増幅・波
形整形され、元のコード信号に変換され、更に測定開始
の命令信号に戻され、入力バッファ53に送出される。
FIG. 8 is a circuit block diagram showing a specific configuration of the position detection circuit 50. In the same figure, there is J3, and the input Ben 20 mentioned above
When an infrared signal is emitted from the light-emitting diode 25 without indicating the code indicating the start of measurement, the infrared signal is received by the infrared receiving diode 51, further amplified and waveform-shaped by the receiver 52, and converted to the original code. It is converted into a signal, further converted back into a measurement start command signal, and sent to the input buffer 53.

演算処理回路54は入力バッファ53にすt’iif記
命令信号を読み取り、測定開始を認識すると、出力バッ
フ?55を介してマルチプレクサ40へ制御信号を送り
、変換回路30と磁性体118〜llhとの接続を次々
に切替える。該変換回路30により変換された各磁性体
11a〜11hの抵抗値に対応する電圧は、増幅器56
へ入力され、増幅され、更に検波器57で整流されて直
流電圧に変換され、更にアナログ−ディジタル(A/D
)変換器58にてディジタル値に変換δれ入力バッファ
53を介して演算処理回路54に送出される。演算処理
回路54では該ディジタル値を前記制御信号に同期して
読み取り、これらをメモリ59に一時記憶する。更に演
算処理回路54は、これらの中より前記極小値付近の電
圧値を検出し、更に眞記(6)式に従ってX座標値を専
用する。
The arithmetic processing circuit 54 reads the t'iif command signal into the input buffer 53, and when it recognizes the start of measurement, outputs the output buffer? A control signal is sent to the multiplexer 40 via the multiplexer 55, and the connection between the conversion circuit 30 and the magnetic bodies 118 to llh is switched one after another. The voltage corresponding to the resistance value of each of the magnetic bodies 11a to 11h converted by the conversion circuit 30 is supplied to the amplifier 56.
is input to the detector 57, amplified, rectified by a detector 57, converted into a DC voltage, and then converted into an analog-digital (A/D) voltage.
) is converted into a digital value by the converter 58 and sent to the arithmetic processing circuit 54 via the input buffer 53. The arithmetic processing circuit 54 reads the digital values in synchronization with the control signal and temporarily stores them in the memory 59. Further, the arithmetic processing circuit 54 detects a voltage value near the minimum value from among these, and further dedicates the X coordinate value according to Equation (6).

第9図は極小値付近の電圧値を検出覆る処理の流れを、
また第10図は演算処理の流れを示すもので、図中、S
Nはスデップナンバー、C8は抵抗値を測定する磁性体
の番号を示ずスキ1シンナンバー、SDは磁性体の抵抗
値に対応するゲイジタル値を示すサンプリングデータ、
HLは所定の判定レベル、CNは検出された権小値に最
も近い電圧を示J磁性体の番号を示すナンバー、Ml。
Figure 9 shows the process flow for detecting voltage values near the minimum value.
Figure 10 shows the flow of calculation processing, and in the figure, S
N is a step number, C8 is a number that does not indicate the number of the magnetic body whose resistance value is to be measured, and SD is sampling data that indicates a gauge value corresponding to the resistance value of the magnetic body.
HL indicates a predetermined judgment level, CN indicates the voltage closest to the detected minimum value, and J indicates the number of the magnetic material, Ml.

M2はメモリに一時記憶するデータ、[)1 、 [)
2 。
M2 is data temporarily stored in memory, [)1, [)
2.

C3、C4、DSはそれぞれ番号が、(CN−2)。C3, C4, and DS each have a number (CN-2).

(CN−1)、(CN)、(CN+1>、(CN+2)
の磁性体の抵抗値を測定した時にサンプリングされたデ
ータである。
(CN-1), (CN), (CN+1>, (CN+2)
This is data sampled when measuring the resistance value of a magnetic material.

このようにして求められたディジタル値のX座標値は、
一旦、メモリ59に記憶されるが、前記測定開始を示す
信号が出されている間、上述したような測定及び演算が
所定時間毎に繰返され、その値は更新される。次に、入
力ペン20より位置指定のコードを示す赤外線信号が発
信され、受光ダイオード51、受信機52、入力バッフ
ァ53を介して演算処理回路54に認識されると、その
時点における前記ディジタル値のX座標値が入力値とし
て、出力バッフ760を介してディジタル表示器(図示
せず)に送出され表示され、またはコンピュータ(図示
せず)に送出され処理されたり、あるいはディジタル−
アナログ(D/Δ)変換器61を介してアナログ信号に
変換され処理される。
The X coordinate value of the digital value obtained in this way is
The value is once stored in the memory 59, but while the signal indicating the start of measurement is being issued, the above-mentioned measurement and calculation are repeated at predetermined intervals, and the value is updated. Next, an infrared signal indicating a position designation code is transmitted from the input pen 20, and when recognized by the arithmetic processing circuit 54 via the light receiving diode 51, receiver 52, and input buffer 53, the digital value at that point is The X coordinate value is sent as an input value via output buffer 760 to a digital display (not shown) for display, or to a computer (not shown) for processing, or to be sent to a digital display (not shown) for processing.
It is converted into an analog signal via an analog (D/Δ) converter 61 and processed.

なお、実施例中の磁性体の本数は一例であり、これに限
定されないことはいうまでもない。また磁性体の間隔は
2〜61a11程度であれば比較的精度良く位置検出が
Cきることが実験により確かめられている。また、入力
ペンに使用する磁気発生器も永久磁石に限定されること
はなく電磁石でもよい。
Note that the number of magnetic bodies in the examples is just an example, and it goes without saying that the number is not limited to this. Furthermore, it has been confirmed through experiments that position detection can be performed with relatively high accuracy if the spacing between the magnetic bodies is approximately 2 to 61a11. Further, the magnetic generator used in the input pen is not limited to a permanent magnet, but may also be an electromagnet.

また、前記実施例において、測定開始、位置指定等を示
す信号を入力ペン20から位置検出回路50まで赤外線
信号を用いで伝送したが超音波信号を用いても良い。ま
た、前記測定開始、位置指定等を示す信号は、単にその
タイミングを演算処理回路54に認識させる為のもので
あるから、特に入力ペン20より送ることを要するもの
ではなく、位置検出回路50自体に設けたギーボード、
その他のスイッチ回路より送る如くなしても良い。
Furthermore, in the embodiment described above, signals indicating measurement start, position designation, etc. are transmitted from the input pen 20 to the position detection circuit 50 using infrared signals, but ultrasonic signals may also be used. Furthermore, since the signals indicating the start of measurement, position designation, etc. are simply for making the arithmetic processing circuit 54 recognize the timing, they do not particularly need to be sent from the input pen 20, but are sent from the position detection circuit 50 itself. A ghee board installed in the
The signal may be sent from another switch circuit.

第11図は本発明の他の実施例を示すものである。同図
において、71及び72はX方向及びY方向の位置検出
部、73及び74はX方向及びY方向用の信号選択回路
で、それぞれ前記位置検出部10.信号選択回路40と
同様な構成を有しており(但し、図面では簡略のためそ
の細部については省略する。)、該位置検出部71.7
2についてはその各磁性体がそれぞれX方向及びY方向
に直交する如く、互いに重ね合わされている。
FIG. 11 shows another embodiment of the invention. In the figure, reference numerals 71 and 72 indicate position detection units in the X and Y directions, and 73 and 74 indicate signal selection circuits for the X and Y directions, respectively. It has the same configuration as the signal selection circuit 40 (however, the details are omitted in the drawing for simplicity), and the position detection section 71.7
2, the respective magnetic bodies are superimposed on each other so as to be orthogonal to the X direction and the Y direction, respectively.

また、75は位と検出回路で、X方向及びY方向の位置
検出を交互に行なわせるようにした点を除いて前記位置
゛検出回路50と同様である。従って、この実施例によ
れば、X方向及びY方向の2方向の位置(座標)検出が
容易に出来る。なお、入力ペン、変換回路の構成は前記
実施例と同じで良い。
Further, 75 is a position detection circuit which is similar to the position detection circuit 50 except that position detection in the X direction and the Y direction is performed alternately. Therefore, according to this embodiment, position (coordinate) detection in two directions, the X direction and the Y direction, can be easily performed. Note that the configurations of the input pen and the conversion circuit may be the same as in the previous embodiment.

また、位置検出部71.72については、1枚の絶縁性
基板の表面および裏面に磁性体およびその配線を設ける
ことにより、一体内に構成することもできる。
Further, the position detecting sections 71 and 72 can also be constructed in one piece by providing a magnetic material and its wiring on the front and back surfaces of a single insulating substrate.

(発明の効果) 以上説明したように本発明によれば、磁性体に加わる磁
気バイアス量に応じて変化する抵抗値より位置を検出す
るため、複数の磁性体をほぼ平行に並べるのみで良く、
位置検出部の構成を極めて簡単にすることができる。ま
た、位置検出の為に位置指定用磁気発生器と他の装置と
の聞に信号をやりとりする必要がないためコードレスと
することができ、更にまた、位置指定の為に必要とする
磁気バイアスの量は、数エルステッド(Oe)程度で良
いので、該位置指定用磁気発生器は位置検出部より多少
離しても位置指定が可能であり、位置検出部の裏面から
の位置指定も可能であり、強磁性体以外の金属を入力面
上に載置することもできる。また、検出の際、磁束変化
等を伴わない為、外部への誘導ノイズの発生が少ない。
(Effects of the Invention) As explained above, according to the present invention, in order to detect the position from the resistance value that changes depending on the amount of magnetic bias applied to the magnetic body, it is only necessary to arrange a plurality of magnetic bodies almost in parallel.
The configuration of the position detection section can be extremely simplified. In addition, since there is no need to exchange signals between the position specifying magnetic generator and other devices for position detection, it can be cordless, and furthermore, the magnetic bias required for position specification can be reduced. Since the amount is only about a few oersteds (Oe), the position can be specified even if the position specifying magnetic generator is separated from the position detecting section by some distance, and the position can also be specified from the back side of the position detecting section. Metals other than ferromagnetic materials can also be placed on the input surface. In addition, since there is no change in magnetic flux during detection, less induced noise is generated to the outside.

また、位置検出部をX方向及びY方向に設けたものによ
れば、2次元の位置検出が可能となる等の利点がある。
Further, if the position detecting sections are provided in the X direction and the Y direction, there are advantages such as two-dimensional position detection becomes possible.

【図面の簡単な説明】[Brief explanation of drawings]

図面は本発明の説明に供するものC1第1図は本発明の
主要な構成を示す説明図、第2図は位四指窓用磁気発生
器より磁性体に印加される磁束のようすを示す図、第3
図は磁性体の抵抗値に対応する電圧値の一例を示すグラ
フ、第4図は位置検出部10の具体的な構成を斜視図、
第5図は位置指定用磁気発生器の具体的な構成を示J断
面図、第6図はその電気回路図、第7図は変換回路の具
体的な回路図、第8図は位置検出回路の具体的な構成を
示す回路ブロック図、第9図は極小値付近の電圧値を検
出する処理の流れを示1゛図、第10図は演算処理の流
れを示す図、第11図は本発明の他の実施例を示す説明
図である。 10・・・位置検出部、20・・・位置指定用磁気発生
器、30・・・変換回路、40・・・信号選択回路、5
0・・・位置検出回路、11a〜11h・・・磁性体、
71・・・X方向位置検出部、72・・・Y方向位置検
出部。 特許出願人  株式会社 ワコム 代理人弁理士  古 1)精 孝 lid   Lie X)薗のを標位1 第8図
The drawings serve to explain the present invention.C1: Figure 1 is an explanatory diagram showing the main structure of the present invention; Figure 2 is a diagram showing the state of magnetic flux applied to the magnetic material from the magnetic generator for the index finger window. , 3rd
The figure is a graph showing an example of the voltage value corresponding to the resistance value of the magnetic material, and FIG. 4 is a perspective view of the specific configuration of the position detection unit 10.
Figure 5 is a sectional view showing the specific configuration of the magnetic generator for position designation, Figure 6 is its electrical circuit diagram, Figure 7 is a specific circuit diagram of the conversion circuit, and Figure 8 is the position detection circuit. Figure 9 is a circuit block diagram showing the specific configuration of , Figure 1 is a diagram showing the flow of processing for detecting voltage values near the minimum value, Figure 10 is a diagram showing the flow of calculation processing, and Figure 11 is a diagram showing the flow of processing for detecting voltage values near the minimum value. FIG. 7 is an explanatory diagram showing another embodiment of the invention. DESCRIPTION OF SYMBOLS 10... Position detection part, 20... Magnetic generator for position specification, 30... Conversion circuit, 40... Signal selection circuit, 5
0...Position detection circuit, 11a-11h...Magnetic material,
71...X-direction position detection section, 72...Y-direction position detection section. Patent Applicant Wacom Co., Ltd. Patent Attorney Furu 1) Takashi Lie X) Heading to Sonono 1 Figure 8

Claims (2)

【特許請求の範囲】[Claims] (1)所定間隔隔てて互いにほぼ平行に配列された複数
の長尺の磁性体を備えた位置検出部と、定常的な磁界を
発生する位置指定用磁気発生器と、 導体のインピーダンス値を電気信号に変換する変換回路
と、 該変換回路と前記位置検出部の複数の磁性体とを切替え
接続する信号選択回路と、 前記位置検出部の複数の磁性体のそれぞれに対応した電
気信号から前記位置指定用磁気発生器の指示位置を算出
する位置検出回路とからなる位置検出装置。
(1) A position detection unit equipped with a plurality of long magnetic bodies arranged substantially parallel to each other at predetermined intervals; a position designating magnetic generator that generates a steady magnetic field; a conversion circuit that converts the signal into a signal; a signal selection circuit that switches and connects the conversion circuit and the plurality of magnetic bodies of the position detection section; A position detection device comprising a position detection circuit that calculates the indicated position of a designated magnetic generator.
(2)所定間隔隔てて互いにほぼ平行に配列された複数
の長尺のX方向の磁性体を備えたX方向位置検出部と、 該X方向位置検出部と同様の構成を有し且つこれと重ね
合わされたY方向位置検出部と、定常的な磁界を発生す
る位置指定用磁気発生器と、 導体のインピーダンス値を電気信号に変換する変換回路
と、 該変換回路と前記X方向及びY方向位置検出部の複数の
磁性体とを切替え接続するX方向及びY方向の信号選択
回路と、 前記X方向及びY方向位置検出部の複数の磁性体のそれ
ぞれに対応した電気信号から前記位置指定用磁気発生器
のX方向及びY方向の指示位置を算出する位置検出回路
とからなる 位置検出装置。
(2) an X-direction position detection unit including a plurality of elongated X-direction magnetic bodies arranged substantially parallel to each other at predetermined intervals; A superimposed Y direction position detection section, a position specifying magnetic generator that generates a steady magnetic field, a conversion circuit that converts the impedance value of the conductor into an electrical signal, and the conversion circuit and the X and Y direction positions. an X-direction and Y-direction signal selection circuit that switches and connects the plurality of magnetic bodies of the detection section; and a signal selection circuit for selecting the position specifying magnet from an electric signal corresponding to each of the plurality of magnetic bodies of the X-direction and Y-direction position detection section. A position detection device comprising a position detection circuit that calculates the indicated position of the generator in the X and Y directions.
JP61087195A 1986-04-17 1986-04-17 Position detecting device Pending JPS62245329A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61087195A JPS62245329A (en) 1986-04-17 1986-04-17 Position detecting device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61087195A JPS62245329A (en) 1986-04-17 1986-04-17 Position detecting device

Publications (1)

Publication Number Publication Date
JPS62245329A true JPS62245329A (en) 1987-10-26

Family

ID=13908200

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61087195A Pending JPS62245329A (en) 1986-04-17 1986-04-17 Position detecting device

Country Status (1)

Country Link
JP (1) JPS62245329A (en)

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